|Publication number||US4263920 A|
|Application number||US 06/024,273|
|Publication date||Apr 28, 1981|
|Filing date||Mar 26, 1979|
|Priority date||Mar 25, 1978|
|Also published as||DE2813068A1|
|Publication number||024273, 06024273, US 4263920 A, US 4263920A, US-A-4263920, US4263920 A, US4263920A|
|Inventors||Manfred Tasto, Hermann Schomberg|
|Original Assignee||Manfred Tasto, Hermann Schomberg|
|Export Citation||BiBTeX, EndNote, RefMan|
|Patent Citations (4), Non-Patent Citations (2), Referenced by (69), Classifications (10)|
|External Links: USPTO, USPTO Assignment, Espacenet|
The invention relates to a method of determining the internal structure of a body which is exposed to an electric field which extends between individual electrodes of an electrode array which at least partly surrounds the body, currents which flow between the individual electrodes being measured and electrical resistance values in the individual tubes of flux generated between the electrodes being determined from said currents.
The invention furthermore relates to a device for performing a method in accordance with the invention.
A method of this kind is known from "Proceedings 29th ACEMB", Boston, Mass., 1976. According to this known method, the body to be examined, for example, a human thorax, is arranged between a first and an equally large second electrode, the second electrode being subdivided into an electrode field which consists of rows and columns and which is assembled from individual measuring electrodes. An electric alternating voltage is applied between the first electrode and the individual measuring electrodes, so that an electric field which extends through the body is formed therebetween. The current flowing through the measuring electrodes is then a measure for an electric resistance value of the body in a tube of flux which is situated between a measuring electrode and the first electrode and whose dimensions are determined by the measuring electrode. The body can thus be represented as a matrix of resistance values consisting of rows and columns, so that an image is obtained in a plane perpendicular to the field direction, each row or each column consisting of one-dimensional image data. The data in the second dimension of the body, extending in the direction of a tube of flux, is then lost.
However, it has been found that determination of a two-dimensional or three-dimensional structure distribution in a body is desirable. The invention has for its object to provide a method whereby a two-dimensional or three-dimensional structure distribution of a body exposed to an electric field can be determined.
To this end, the method in accordance with the invention is characterized in that the body is successively exposed to differently directed electric fields, for each field direction electric currents being measured in the individual tubes of flux which occur between the electrodes and which differ for each field direction, after which the measured currents are used to determine resistance values wherefrom specific resistance values in individual elements of a matrix which is imagined in the body exposed to the successive fields, for each field direction the tubes of flux and equipotential lines associated with this field direction being determined at least once from a given distribution of specific resistance values over the elements, after which for each tube of flux an associated resistance value is determined from the given specific resistance distribution, after which each calculated resistance value a correction resistance distribution for the tube of flux is calculated by determination of the difference with respect to the resistance value measured in the associated tube of flux, a correction for the specific resistance value for each element being calculated from said correction resistance distributions by interpolation.
This method enables determination of a two-dimensional or three-dimensional structure distribution, for example, a distribution of the specific resistance, in a body exposed to an electric field, for example, a resistance distribution of a human thorax or of an arm. To this end, the specific resistance of the body is determined in individual elements of a matrix which is imagined in the body, it being possible, for example, to convert the individual values of the specific resistance into corresponding grey values for the display of a resistance distribution in a plane on a monitor.
The given resistance distribution to be used for the method is either a resistance distribution determined from a preceeding calculation or a distribution selected on the basis of an anatomical atlas, so that the resistance distribution to be ultimately calculated is closely approximated and the corrections following from the calculations are not excessively large. It has been found that this is advantageous, because the number of iterations to be executed per field direction is thus limited.
In many cases it is not necessary to determine a three-dimensional structure distribution of a body, so that it suffices to produce a specific resistance distribution in a plane of the body exposed to the field. The amount of work and hence the time required for determining the distribution of the specific resistance for the examination of the body is thus reduced.
One version of the method in accordance with the invention is characterized in that the electrode array is rotated around an axis which extends through the body, said axis being constantly directed transversely of the electric field generated between the electrodes, a position thereof remaining unchanged with respect to each electrode.
It is thus achieved that during rotation of the electrode array around the body, the electric field always extends in the same plane and that the electrode array always occupies a prescribed position, which is necessary for the reconstruction of an internal structure of a body being examined from the measurement. The electrical contact between the electrodes and the body can be realized via an electrolyte which surrounds the body to be examined and whose specified resistance is known and does not excessively deviate from the specific resistance of the body to be examined. If the body to be examined is, for example, part of a human body, the electrolyte may be water.
The direction of the field can alternatively be reversed by pole reversal of all electrodes of the electrode array. It is thus achieved that the electrode device need no longer be rotated fully around the body to be examined. If the sense of rotation of the field is reversed for each direction of the electric field, rotation of the electrode array through an angle of, for example, 180° actually suffices for the execution of resistance measurements in all directions within an angle of 360°. The time required for measuring the resistance values along the individual tubes of flux can thus be substantially cut in half.
A further version of a method in accordance with the invention is characterized in that the successively differently directed fields are generated by pole reversal of individual electrodes of the electrode array, the position of the electrode array remaining unchanged with respect to the body to be examined. In order to enable the electrical field to assume any direction in the plane of the body to be examined, the body is fully enclosed by individual electrodes which are situated in the plane, the polarity of said electrodes being changed each time so that a rotation is realized of the field direction between the individual electrodes which are stationary with respect to the body. In order to avoid an excessive potential difference from arising between neighbouring individual electrodes of different polarity, the voltage present on the individual electrodes can be reduced in the direction of the polarity difference from electrode to electrode. Because rotation of the electrode array with respect to the body is avoided, the time required for measuring the resistance values in the individual tubes of flux can be minimized.
According to a further version of a method in accordance with the invention, the electrode are connected to an alternating voltage in order to generate the field between individual electrodes of the electrode array. As a result, polarization of a body present between the individual electrodes is avoided.
The invention also relates to a device for performing the method in accordance with the invention, comprising a power supply source and an electrode array for generating an electric field, at least part of the electrodes of said electrode array being connected to a measuring system for measuring currents flowing through the individual electrodes, said currents being a measure for the resistance values of tubes of flux generated between electrodes of different polarity, a memory for the storage of values obtained and a display device for the display of values obtained, characterized in that the device comprises means for generating successive electric fields in different directions by means of the electrode array, all fields being directed substantially transversely of an axis extending through the body, the measuring system being suitable for measuring the currents flowing through the individual electrodes at the different field directions, said device furthermore comprising a first storage section for the storage of values which are a measure for the direction of the successive fields and for storing the resistance values to be derived from the currents measured which are associated with the direction of the field generating the currents, a second storage section for the storage of specific resistance values, each of which is associated with one element of a matrix of elements, a third storage section for the storage of further data, and a central processor unit:
for determining from the specific resistance values and for a given field direction, field and equipotential lines which subdivide a space defined by the matrix into meshes, values which determine dimensions of the meshs being stored in the third storage section,
for determining, by interpolation, a specific resistance in each mesh from the specific resistance values in the elements on the basis of given coordinates of each mesh, said specific resistance being stored in the third storage section,
for calculating a resistance value between two field lines by summation of mesh resistance values which are directly proportional to the specific resistance and the length and inversely proportional to the width of the associated mesh,
for determining, from the difference between the resistance value measured and calculated for the given field direction, a correction resistance distribution per mesh which is directly proportional to said difference and to the length and inversely proportional to the width of the mesh, said correction resistance distribution being stored in the third storage section;
for determining, by interpolation, from the correction resistance distribution a correction for the specific resistance values in each element,
for adding the correction to the associated specific resistance value, a sum thus obtained being stored in the second storage section.
The invention will be described in detail hereinafter, with reference to the accompanying diagrammatic drawing.
FIG. 1 shows a box-like electrode array for the description of the method,
FIG. 2 is a plan view of the electrode array shown in FIG. 1 with electrical measuring and power supply elements,
FIG. 3 shows a hypothetical body to be examined,
FIG. 4 shows and electrode array with a body to be examined.
FIG. 5 shows a network, formed by equipotential lines and field lines, in a plane in an electrode array in accordance with FIG. 1,
FIG. 6 shows, at an increased scale, a mesh of the network formed by equipotential lines and field lines of FIG. 5,
FIG. 7 shows a matrix which is permanently related to the body to be examined and which is situated in the plane subject to the electric field,
FIG. 8 illustrates an interpolation to be used for the method,
FIG. 9 illustrates a further interpolation,
FIG. 10 shows a box-like electrode array,
FIGS. 11a and 11b each are a sectional view of an electrode array in which a body is arranged in order to illustrate the course of the electrode field lines,
FIG. 12 is a block diagram of a device for performing the method in accordance with the invention,
FIG. 13 shows a ring-like electrode array,
FIGS. 14a, b, c each show a plane which is subject to an electric field in a box-like electrode array, the field occupying different directions in the plane,
FIG. 15 shows a cylindrical array which is to be arranged around a body and which comprises individual electrodes to be arranged on the body, and
FIG. 16 shows an elastic electrode array which is to be arranged closely against the body.
The method of determining a structural distribution of a body will be described in detail hereinafter on the basis of a two-dimensional example. The method can be readily extended to three dimensions by taking into account each time the associated third coordinate in the following equations.
FIGS. 1 to 9 serve for the description of the method.
The plane of the body to be examined is surrounded by an electrode array which is situated in two parallel planes, so that the plane of the body to be examined is situated completely in the electric field extending between the electrodes of the electrode array. The electrode array comprises individual, adjacently arranged electrodes, the position of which in the plane is at least approximately known, so that tubes of flux are generated in accordance with the dimensions of the individual electrodes, said tubes being adjacently situated inside the body. The body is successively exposed to an electric field which is generated in different directions in the plane, so that currents are generated and measured in the individual tubes of flux. From the currents measured, electric resistance values are determined in the various tubes of flux, wherefrom subsequently the specific resistance is determined in individual elements of a matrix which is permanently related to the body and which is situated in the plane exposed to the electric field. The determination of the specific resistance will be described in detail hereinafter. The dimensions of the tubes of flux and hence the resolution of the electrode array are determined by the surface area of the individual measuring electrodes.
FIG. 1 shows a box-like electrode array which comprises a tank 1 which is to be filled with an electrolyte and whose walls 2, 3, 4, 5 and bottom 6 are made of an electrically insulating material. The electrode array consists of a strip-like electrode E which is arranged against the inner side of the rear wall 5 and which corresponds to the dimensions of the rear wall 5 and of various individual, rectangular electrodes Em are equally large and which are arranged against the inner side of the front wall 3. The individual electrodes Em cover the front wall 3 and are electrically insulated with respect to each other. The number of individual measuring electrodes Em amounts to M. In this example, M has the value eight. The walls 2,3, 4 and 5 each have a length 2r and a height h.
Furthermore, a rectangular coordinate system [ξ, η, ζ] is permanently related to the tank 1, the coordinate axes thereof extending perpendicularly through the walls 2, 3, 4 and 5 and the bottom 6, the origin 7 of said coordinate system being situated in a centre of the tank 1. The ξ-direction extends parallel to the electrode E and the ζ-direction extends perpendicular to the bottom 6.
FIG. 2 is a plan view of the tank 1. The individual measuring electrodes Em are each connected in series to current measuring apparatus Sm which have a low internal resistance and which are all connected, via a voltage source 9, to the electrode E. Electrically parallel connected to the voltage source 9 is a voltage measuring apparatus 10 which measured approximately the electric voltage drop U between the strip-like electrode E and the individual measuring electrodes Em. (Further circuit components have been omitted for the sake of simplicity).
FIG. 3 shows a body 11 to be examined which is to be arranged in the tank 1 and which is situated in the origin 12 of a Cartesian coordinate system [x, y, z] which is permanently related thereto. The body 11 is shaped so that the geometry does not change in the z-direction. Furthermore, it is assumed that the specific resistance ρ(x, y, z), capable of assuming values in the range 0<ρ(x, y, z)<∞, is at least approximately independent of the z-direction and of electric and magnetic fields. The height of the body 11 in the z-direction corresponds to the height h of the tank 1.
FIG. 4 is a sectional view of the tank 1 in the ξ-η plane of the coordinate system [ξ, η, ζ] which is associated with the tank 1. The body 11 to be examined is arranged inside the tank 1 so that the origins 7, 12 and the ζ and z-directions of the two systems of coordinates [ξ, η, ζ], [x, y, z], respectively, coincide. The body 11 can be rotated with respect to the tank 1 in that either the body 11 is rotated around the z-axis in the stationary tank 1, or in that the tank 1 is rotated around the z-axis whilst the body 11 is stationary. The ξ and x-directions then enclose an angle θ which always indicates the position of the body 11 with respect to the tank 1. The electrolyte 13, having a specific resistance ρb is present around the body 11. The electrolyte 13 is chosen so that the specific resistance ρb thereof at least approximately corresponds to the specific resistance ρ(x, y, z) of the body 11. The circle 14 denoted by a broken line in the tank 1 bounds the largest area which may be occupied by a body 11 during a relative movement between the body and the tank 1. The area occupied by the body 11 in the ξ-η plane will be referred to as the object area D hereinafter.
Using the assumptions made concerning the z-independency of contour geometry and specific resistance ρ(x, y, z) of the body 11, the problem has been reduced to two dimensions, so that hereinafter it is merely necessary to consider only the relationships in the ξ-η plane of the coordinate system [ξ, η, ζ] permanently associated with the tank 1. Such a consideration of the problem is possible for a very small height h of the tank.
For determining the two-dimensional structural distribution in the object area D of the body 11, a voltage U is applied between the strip-like electrode E and the individual measuring electrodes Em (E1, . . . ,EM). For each tube of flux 17, defined by the dimensions of the electrodes Em (FIG. 5), the electric current Imθ flowing therethrough is measured, said current being dependent of the mth measuring electrode Em and of the angle θ which indicates the position of the body 11 with respect to the tank 1.
Thus, a so-termed current projection (I1θ . . . IMθ)for an angle θ is obtained. The vector (R1θ . . . RMθ) then represents the associated resistance projection for the angle θ at which an individually measured resistance value Rmθ =U/Imθ. In order to enable accurate determination of the distribution of the specific resistance ρ(x, y, z) in the area D of the object, it is necessary to record resistance projections at different angles θn. Thus, a set of resistance projections is obtained: ##EQU1## associated with a set of angles θn, where n=1, . . . ,N. Hereinafter, the angle θn is only referred to as n, θn assuming values in the range 0≦θn <2π. The invention has for its object to determine the specific resistance ρ(x, y, z) in the object area D of the body 11 by means of these resistance projections. To this end, a given (assumed) resistance distribution within the object area D is required, as will be explained hereinafter.
FIG. 5 again shows the ξ-η plane extending through the tank 1. When a voltage U is applied between the strip-like electrode E and the individual measuring electrodes Em, a network 16 consisting of electric field lines 14 and equipotential lines 15 is imagined in the tank 1, in accordance with the distribution of the specific resistances ρb and ρ(x, y, z) of the electrolyte 13 and the body 11. Two field lines 15 each time enclose a tube of flux 17.
For determining calculated resistance values Rmn i, it makes sense to subdivide a tube of flux 17 into different meshes Qmn.sup.μ, each mesh Qmn.sup.μ being bounded by two equipotential lines 15 and two field lines 14. The number of meshes may be chosen to correspond to the number of electrodes Em, each mesh Qmn.sup.μ having a mesh resistance Rmn.sup.μ, μ being the number of mesh in a tube of flux 17 (0≦μ≦M). The resistance value Rmn i for each tube of flux 17 is then found by summing the mesh resistances Rmn.sup.μ of all meshes Qmn.sup.μ, where Rmn i =Σ.sub.μ Rmn.sup.μ and μ=1, . . . ,M.
FIG. 6 is a representation at an increased scale of a mesh Qmn.sup.μ with an arrow 18 which indicates the field direction. The mesh Qmn.sup.μ is bounded by two field lines 14 and two equipotential lines 15 which intersect at the corner points P1, P2, P3, P4 of the mesh. A rectangle 19, having a width wmn.sup.μ and a length 1mn.sup.μ is arranged across the mesh Qmn.sup.μ. The determination of the resistance data can thus be substantially simplified. Taking into account the small height h of the tube of flux 17, the following expression is obtained for a tube of flux 17: ##EQU2## Therein, the mesh resistance Rmn.sup.μ is given by the specific resistance ρmn.sup.μ at the point Pmn.sup.μ, the point Pmn.sup.μ being situated in the centre of the rectangle 19.
The rectangle 19 is formed as follows. Two corner points P1, P2, P3, P4 of the mesh are interconnected by a straight lines on which points P12, P23, P34, P14 are indicated which are situated halfway between two corner points P1, P2, P3, P4 of the mesh. The sides of the rectangle 19 are arranged through the points P12, P23, P34 and P14.
Taking into account that the body 11 is situated only in the area D of the object, the resistance value Rm for each tube of flux 17 amounts to: ##EQU3## Therein, the outer region D (FIG. 4) of the tank 1 which surrounds the object area D contains the electrolyte 13 having a specific resistance ρb. It is to be noted that neither the length 1mn.sup.μ, nor the width wmn.sup.μ, nor the specific resistance ρmn.sup.μ or the location of the point ρmn.sup.μ are known, because the course of the field lines 14 and the course of the equipotential lines 15 in the tank 1 is unknown.
In order to solve the problem concerning the specific resistance ρmn.sup.μ, the x-y plane of the system of coordinates x, y, z relates to the body 11 is covered by a matrix P as shown in FIG. 7. A raster P of this kind also has a fixed positional relation with respect to the body 11. The individual points Pij in the matrix P have the coordinates (iΔ,jΔ,0) and are the centres of the elements εij. Therein, Δ=2r/M and i and j are a running index (i, j=-M/2, . . . 1, 0, 1, 2 . . . +M/2). In the elements εij it is then possible to define new specific resistance ρij which are unknown per se but which can be readily determined. Each point Pmn.sup.μ (FIGS. 5,6) is surrounded by four points Pij, so that an approximate specific resistance ρmn.sup.μ at the point Pmn.sup.μ can be determined by bilinear interpolation from the specific resistance ρij. Of course, this is necessary only in the object area D, because the specific resistance ρb in the outer region D in any location is known.
FIG. 8 serves to illustrate the bilinear interpolation. At a point P (for example, Pmn.sup.μ), the specific resistance ρmn.sup.μ is to be determined. The point P obtains the assumed coordinates (x, y, 0) within the object area D. First a pair of indices i, j is determined for which the relation xi ≦x≦xi+1 and yj ≦y≦yj+1 is applicable. Thus, the four points Pij of the matrix P surrounding (x, y, 0) are determined. Subsequently, ρmn.sup.μ is determined in accordance with the equation: ##EQU4## Therein, α=(x-xi)/Δ and β=(y-yi)/Δ. In the vicinity of the edge of the object area D, some points: Pij ; Pi+1,j ; Pi,j+1 ; Pi+1,j+1 may be situated outside theobject area D. In that case the specific resistance ρmn.sup.μ is assumed to be equal to the specific resistance ρb of the electrolyte 13.
The length 1mn.sup.μ and the width wmn.sup.μ of the rectangle 19 and the coefficients α,β are dependent of the course of the field lines 14 and the equipotential lines 15 in the system of coordinates [ξ, η, ι], the course again being determined by the distribution of specific resistance ρ(x, y, z) of the body 11 which encloses an angle θn with respect to the tank 1. Even though the distribution of specific resistance ρ(x, y, z) in the body 11 is unknown, the length 1mn.sup.μ, the width wmn.sup.μ and the coefficients α and β can be determined if a specific resistance ρij is given at the points Pij of the object area d of the matrix P permanently related to the body 11. The values of the specificresistance ρij are continued, by linear interpolation, to a function in the x-y plane, wherefrom a function of a specific resistance ρ.sub.θn, defined in the ξ-η plane, can be determined by means of a simple coordinate transformation. Using known electrostatics equations and taking into account the secondary conditions, the aproximate course of the field lines 14 and equipotential lines 15 in the ξ-η plane can be determined from the function of this specific resistance ρ.sub.θn, it being possible to determined the length 1mn.sup.μ and the width wmn.sup.μ and the coefficients α and β from this course. Of course, this is applicable to each angle θn and to each set of specific resistances ρij and each set of points Pij of the elements εij of the matrix P.
Only the specific resistance ρij at the points Pij of the matrix P is known. However, this can be given in advance, for example, by assuming it to be equal at all points Pij to the specific resistance ρb. The first approximation of the specific resistance ρij is then stepwise improved, in that each time for all tubes of flux 17 the calculated resistance values Rmn i are compared with the measured resistance values Rmn for correction of the specific resistance ρij, correction values Δρij for ρij being determined therefrom.
Assume that the method has proceeded to the step k (k=integer number). In this kth step, a distribution of the specific resistance ρij k (at the points Pij of the matrix P) is given in advance. The aim is then to obtain the distribution of the specific resistance ρij k+1 for the beginning of the (k+1)th step. Furthermore, an angle θ.sbsb.nk is chosen at which the body 11 extends with respect to the tank 1, so that the data ρij k and θn.sbsb.k can be determined from the course of the field lines 14 and the course of the equipotential lines 15 by using known electrostatic equations and taking into account the secondary conditions (the voltage applied to the electrodes). From the course of the field lines and equipotential lines, a set of cross-points ##EQU5## of field lines 14 and equipotential lines 15 is derived; therefrom the length 1 mn.sbsb.k.sup.μk, the width wmn.sbsb.k.sup.μk and the point Pmn.sbsb.k.sup.μk of a rectangle assumed on a mesh Qmn.sbsb.k.sup.μk (see FIG. 6) can be readily derived. The cross-points [ξmn.sbsb.k.sup.μk , ηmn.sbsb.k.sup.μk ] then correspond to the corner points P1, P2, P3, P4 of the mesh in FIG. 6.
Subsequently, the specific resistance ρmn.sbsb.k.sup.μk at point Pmn.sbsb.k.sup.μk is determined from ρij k by bilinear interpolation. The bilinear inerpolation has already been described with reference to FIG. 8. Using these data, the resistance values Rmn.sbsb.kk can be determined in the kth step via the following calculation: ##EQU6## in which m extends from 1 up to and including M.
Hereinafter, various calculated resistance values Rmn.sbsb.kk in general fo the measured resistances Rmn.sbsb.k will be given. Therefore, for each point Pmn.sbsb.k.sup.μk of the object area D a correction Δρmn.sbsb.k.sup.μk for the previously determined specific resistance ρmn.sbsb.k.sup.μk is determined. This correction is directly proportional to the length 1mn.sbsb.k.sup.μk and inversely proportional to the width wmn.sbsb..sup.μk. The proportionality factor is determined via a formula as follows: ##EQU7## Thus, for the k+1)th step a distribution of the specific resistance ##EQU8## is obtained for the points Pmn.sbsb.k.sup.μk in the meshes Qmn.sbsb.k.sup.μk.
However, it is important to determine the change Δρij k of the specific resistance ρij k in the elements εij of the matrix P in the object area D. The change Δρij k is determined by interpolation between the corrections Δρmn.sbsb.k.sup.μk is obtained.
FIG. 9 illustrates the interpolation method. A point Pij in the object area D is given. First a polygon Qmn.sbsb.k.sup.μk, comprising corner points Pmn.sbsb.k.sup.μk, Pm+1,n.sbsb.k, Pm+1,n.sbsb.k.sup.(μ+1)k and Pm,n.sbsb.k.sup.(μ+1)k, wherebetween Pij is situated, is searched. Subsequently, the position of the points P1 and P2 is determined by extending two lines a and b so that they intersect in a point c. Through the points c and Pij a third line is drawn whose points of intersection with lines e and f determine the position of the points P1 and P2. Linear one-dimensional interpolation in the direction of the lines e and f is used to determine the intermediate values Δρp1, and Δρp2 and therefrom the change Δρij k by linear one-dimensional interpolation again. If the polygon Qmn.sbsb.kuk is a rectangle, the preceding interpolation is reduced to a normal bilinear interpolation. The kth step has been completed after calculation of the new specific resistance ρij k +1 =ρij k +Δρij k for all i and j which are associated with the elements εij which are situated in the object ar D. For the next step a new angle θn.sbsb.k +1 is chosen which effectively deviates of from 45° to 90° from the angle θn.sbsb.k. The calculations may be interrupted, for example, after a given number of iterations k, for example, the measuring values measured at all angles θn being used a corresponding number of times in the calculation.
FIG. 10 is a broken-away view of a box-like tank 31 by means of which a body 32 to be examined can be examined in different planes 20 which are denoted by broken lines. A plane 20 is the ξη plane or the x-y plane described with reference to FIG. 4. On the inner side of the tank wall 33 there are provided various strip-like electrodes E which have a height h and whose longitudinal direction L extends perpendicular to the symmetry axis 21 of the tank 31 which is assumed to be the axis of rotation. The axis of rotation 21 is actually the ζ or z-axis shown in the FIGS. 1 and 3, respectively. On the tank wall 34 (only partly shown) which is situated opposite the tank wall 33 there are provided similarly arranged but individual measuring electrodes Em, so that an electrode field consisting of rows and columns is formed. Between the strip-like electrodes E and the measuring electrodes Em a flat electric field is produced when an external voltage is applied, the direction of said field being represented by the arrow 22. Above and below the electrodes E and the measuring electrodes Em there are provided further strip-like guard electrodes G which are arranged in the same way as the strip-like electrodes E in order to ensure that the field F between the electrodes E and Em does not expand in the direction of the axis 21. At the upper side and the lower side of the tank 1 there is provided an elastic cover 23 with an aperture 25 and a collar 24 wherethrough a body 32 to be examined can be introduced into the tank 1. The elastic cover 23 should comprise rotatable seals (not shown) so that the collar 24, flatly contacting the body 32 so that the electrolyte 35 surrounding the body 32 cannot escape from the tank 31, can be stationary whilst the tank 31 rotates. It is to be noted that all electrodes E and guard electrodes G carry the same potential.
A further embodiment of the tank 31 comprises a single electrode plate (not shown) which is arranged on the inner side of the tank wall 33 and completely covers this wall and which comprises all strip-like electrodes E and guard electrodes G.
In order to obtain an approximation where the contour of the body 32 or the specific resistance ρ(x, y, z) thereof may be independently considered in the z-direction (longitudinal direction of the axis of rotation 21), the height h of the measuring electrodes Em and of the strip-like electrodes E should be small accordingly.
The function of the guard electrodes G will be described with reference to the FIGS. 11a and b. In the absence of guard electrode G (FIG. 11a), the field F (field lines denoted by broken lines) present between the electrode E and the electrodes Em at the area of the body 32 will expand beyond the electrodes E and Em. As a result of the use of guard electrodes G (FIG. 11b), the field F at the area of the individual electrodes Em is maintained at least approximately in the plane between the electrodes E and Em.
FIG. 12 shows an embodiment of a device for performing (in cooperation with, for example, the measuring tank shown in FIG. 10) the method in accordance with the invention. The voltage source 9, the voltmeter 10, the ammeters S1, S2, . . . Sm, and the measuring electrodes E1, E2, . . . Em . . . EM shown in FIG. 10 form a measuring system whose outputs which carry measuring values are all connected to a first processing circuit 25 which may comprise, for example, an analog multiplex circuit and an analog/digital converter The circuit 25 has connected to it an angle measuring device 26 which supplies a measuring value which is directly proportional to the angular shift of the tank 31 with respect to the stationary body 32 to be examined. The angle measuring device 26 may be, for example, a multiturn potentiometer which is mechanically coupled to the tank 31 in known manner.
Under the control of a central processor unit 27, the measuring values applied to the circuit 25 are stored in a magnetic tape memory 28 in digital form. After all measuring values have been collected, the central processor unit 27 calculates the values Rmn and θn which are stored in a first storage section 30a.
Using given specific resistance values ρij, stored in advance in a second storage section 30c, the course of a number of field lines and equipotential lines occurring in a plane 20 defined by the tank 31 are calculated for an angle θn to be selected (from storage section 30a), the number of field lines (M) being determined by the number of measuring electrodes EM. The number of equipotential lines is preferably chosen to equal M. From the cross-points of the field and equipotential lines to be determined, the dimensions (for example, length l/mn.sbsb.k.sup.μk, width w/mn.sbsb.k.sup.μk) are derived for the meshes Q/mn.sbsb.k.sup.μk which are enclosed by the field lines and equipotential lines. By interpolation of the dimensions of the meshes Q/mn.sbsb.k.sup.μk and the given ρij, significant resistance values ρ/mn.sbsb.k.sup.μk are obtained for the meshes, said specific resistance values being stored in a storage section 30b together with the dimensions of the meshes. The coordinates of the corner points (the cross-points of the field and equipotential lines) are also stored in the storage section 30b. If the capacity of the storage section 30b is to be limited, it is alternatively possible to store only said coordinates; in that case, however, distances between the coordinates must each time be calculated again for each calculation.
Using the dimensions and specific resistance values ρ/mn.sbsb.k.sup.μk stored in the storage section 30b, a resistance value Rmn.sbsb.kk is calculated for each tube of flux by means of the formula (5). Subsequently, after the fetching of the values Rmn from the storage section 30a and the dimensions of the various meshes Q/mn.sbsb.k.sup.μk is from the storage section 30b, a correction resistance distribution Δρ/mn.sbsb.k.sup.μk is determined by means of the formula (6). The correction resistance distribution Δρ/mn.sbsb.k.sup.μk is stored in the storage section 30b at the location of the specific resistance value ρ/mn.sbsb.k.sup.μk. Subsequently, the values Δρ/mn.sbsb.k.sup.μk (see FIG. 9 and associated description) are interpolated to form a correction Δρij k which is added to the previous value ρij k. The sum is the new specific resistance ρij k+1 which is stored in the storage section 30c. After a sufficient number of iterations have been performed for each measuring direction θ n, the calculated specific resistance values ρij k+1 can be displayed on a display device 29. If necessary, these values can be recorded e.g. in a punched tape (not shown) or on a magnetic disc memory. After calculation of all ρij k+1, a next measuring direction θn is chosen for which the field and equipotential lines are again calculated on the bases of the corrected ρij k+1. After all measuring values Rmn of each measuring direction θn have been used, the measuring values Rmn of a previously treated measuring direction θn can be used again, using the ρij k+1 corrected thus far.
The number of iterations to be performed for each measuring direction θn may be indicated in advance, but it may also be made dependent of the difference between the measured resistance values Rmn and the calculated resistance values Rmn.sbsb.kk.
FIG. 13 shows a tank 51, the walls 52, 53, 54, 55 of which support a strip-like ring of electrodes Er on their inner side, said ring having a limited height h and being arranged in a plane (FIG. 10) which extends perpendicularly to the axis of rotation 56. Each of the electrodes Er may be connected to a positive or a negative pole of a voltage source as desired. Above and below the individual electrodes Er each time individual rectangular guard electrodes Gm are provided, the width in the direction U thereof corresponding to the width of the individual electrodes Er. Pole reversal of individual electrodes Er and associated guard electrodes Gm enables the direction of the field F generated between the electrodes Er can be changed with respect to a body to be arranged in the tank 51 without relative movement between tank 51 and the body. The change of the polarity of the guard electrodes Gm should each time correspond to that of the individual electrodes Er.
FIGS. 14a, b, c are sectional views through the individual electrodes Er, perpendicularly to the axis of rotation 56 of the tank 51. Two coherent groups of individual electrodes Er have a positive or a negative polarity. By changing the polarity of one of the outer individual electrodes Er of each group, the direction 57 of the field F with respect to the tank 51 or with respect to the body (not shown) can be rotated through an angle which is determined by the dimensions of the electrode. In the vicinity of the tank wall 52, 53, 54, 55, only a "shift" of the field F occurs, because the field always extends perpendicularly to the surface of the individual electrodes Er, so that the object area D (FIG. 4) should be chosen smaller accordingly.
Obviously, the tank 51 may also be shaped as a circle cylinder, so that the maximum permissible object area D (FIG. 4) may be larger.
The changing of the direction 57 of the electric field F is realized by pole reversal of the individual electrodes Er, each of which is connected to switching means 58 (shown only for two electrodes), said switching means being connected to power supply lines 59. The supply lines 59 are connected to a voltage source (for example, as shown in FIG. 10). Activation of the switching means 58 causes pole reversal of the electrodes Er connected thereto, so that an electric field F is generated as shown in FIG. 14b.
Obviously, the switching means 58 may be not only manual switches, as shown, but may also consist of electromagnetic or semiconductor switches, so that a substantially higher switching speed can be obtained. It is thus possible on the one hand to reduce the measuring time (time necessary for measuring in each feasible field with a different direction) and on the other hand, utiliziing an accurately stabilized direct voltage source, and still operating the electrode array with "alternating voltage" (by a high switching frequency of the switching means) in order to avoid polarization of an object arranged between the electrodes.
FIG. 15 shows a rigid, cylindrical ring 60 of a tank 61, formed as a hollow cylinder, which is provided with single electrodes Ee. The single electrodes Ee are rod-shaped, and one end thereof comprises a contact area 62 which is arranged directly on the surface of the body 63 to be examined. To this end, the single electrodes Ee are arranged on the ring 60 to be displaceable in the radial direction with respect to the body 63. All single electrodes Ee also comprise measuring elements (not shown) which determine the displacement of the single electrodes Ee and hence the position of the contact areas 62. The guard electrodes which are situated above and below the single electrodes Ee and which are shaped and arranged on the ring 60 in the same way as single electrodes Ee, have been omitted for the sake of clarity.
The ring 60 consists of two separate ring halves 60a and 60b which are rotatable about a connection shaft 64, so that the ring can be arranged around the body 63.
In FIG. 16, the tank 71 is shaped as an elastic hollow cylinder 73 which is to be arranged flatly against the body 72 and the inner side of which supports individual electrodes Em as well as guard electrodes Gm which are also made of an elastic, electrically conductive material. The arrangement of the individual electrodes Em as well as of the guard electrodes Gm corresponds to that of the electrodes Er and Gm, respectively, of the tank 51 described with reference to FIG. 13 which is constructed as a rigid, square cylinder.
When a body to be examined consists of a dielectric which is substantially not conductive, the described method can be used, for example, to determine a flat distribution of a dielectric constant of the body (for example, material tests), preferably by means of a tank 51 as described with reference to FIG. 13, by applying a high frequency alternating voltage to the individual electrodes Er. Capacitance projections (projection of apparent resistances) (x10, . . . xMθ), where xm is U/Im =1/(2.f.Cm), corresponding to "resistance projections" (R1θ. . . RMθ), can be determined by measuring the currents flowing through the electrodes Er or the electric voltages present therebetween. In that case, no conductive electrolyte 13 need be present between the tank walls 52, 53, 54, 55 and a body to be examined. The determination of the flat distribution of the dielectric constants is then realized in the already described manner.
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|U.S. Classification||600/547, 73/172|
|International Classification||A61B5/0408, G01R27/02, A61B5/05, A61B5/053, G01N27/00|
|Cooperative Classification||A61B5/0536, A61B5/04085|